Breakdown of the Nagaoka phase at finite doping
arXiv:1612.03646 · doi:10.1103/PhysRevB.95.155115
Abstract
The Nagaoka () limit of the Hubbard model on a square lattice is mapped onto the itinerant-localized Kondo model at infinitely strong coupling. Such a model is well suited to perform quantum Monte Carlo (QMC) simulations to compute spin correlation functions. This model is shown to exhibit no short-range ferromagnetic (FM) spin correlations at any doping and finite temperature, . Our simulations give no indication that there is a tendency towards ferromagnetic ordering in the ground state.
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Cited by in corpus (8)
- Polaronic mechanism of Nagaoka ferromagnetism in Hubbard models
- Magnetic phase diagram of the infinite-U Hubbard model with nearest- and next nearest-neighbor hoppings
- Onset of ferromagnetism for strongly correlated electrons in one-dimensional chains
- Stable and Metastable Kinetic Ferromagnetism on a Ring
- Functional renormalization group for extremely correlated electrons
- Shaping Magnetic Order by Local Frustration for Itinerant Fermions on a Graph
- Bad Metal Behavior and Lifshitz Transition of a Nagaoka Ferromagnet
- Itinerant magnetism in Hubbard models with long-range interactions